The SEGUE K Giant Survey. II. Distances of 6036 Stars (Xue+, 2014)
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Arxiv:1303.1406V1 [Astro-Ph.HE] 6 Mar 2013 the flux of Gamma-Rays from Dark Matter Annihilation Takes a Surprisingly Simple Form 2
4th Fermi Symposium : Monterey, CA : 28 Oct-2 Nov 2012 1 The VERITAS Dark Matter Program Alex Geringer-Sameth∗ for the VERITAS Collaboration Department of Physics, Brown University, 182 Hope St., Providence, RI 02912 The VERITAS array of Cherenkov telescopes, designed for the detection of gamma-rays in the 100 GeV-10 TeV energy range, performs dark matter searches over a wide variety of targets. VERITAS continues to carry out focused observations of dwarf spheroidal galaxies in the Local Group, of the Milky Way galactic center, and of Fermi-LAT unidentified sources. This report presents our extensive observations of these targets, new statistical techniques, and current constraints on dark matter particle physics derived from these observations. 1. Introduction Earth's atmosphere as a target for high-energy cosmic particles. An incoming gamma-ray may interact in the The characterization of dark matter beyond its Earth's atmosphere, initiating a shower of secondary gravitational interactions is currently a central task particles that travel at speeds greater than the local of modern particle physics. A generic and well- (in air) speed of light. This entails the emission of motivated dark matter candidate is a weakly in- ultraviolet Cherenkov radiation. The four telescopes teracting massive particle (WIMP). Such particles of the VERITAS array capture images of the shower have masses in the GeV-TeV range and may inter- using this Cherenkov light. The images are analyzed act with the Standard Model through the weak force. to reconstruct the direction of the original particle as Searches for WIMPs are performed at particle accel- well as its energy. -
Two Stellar Components in the Halo of the Milky Way
1 Two stellar components in the halo of the Milky Way Daniela Carollo1,2,3,5, Timothy C. Beers2,3, Young Sun Lee2,3, Masashi Chiba4, John E. Norris5 , Ronald Wilhelm6, Thirupathi Sivarani2,3, Brian Marsteller2,3, Jeffrey A. Munn7, Coryn A. L. Bailer-Jones8, Paola Re Fiorentin8,9, & Donald G. York10,11 1INAF - Osservatorio Astronomico di Torino, 10025 Pino Torinese, Italy, 2Department of Physics & Astronomy, Center for the Study of Cosmic Evolution, 3Joint Institute for Nuclear Astrophysics, Michigan State University, E. Lansing, MI 48824, USA, 4Astronomical Institute, Tohoku University, Sendai 980-8578, Japan, 5Research School of Astronomy & Astrophysics, The Australian National University, Mount Stromlo Observatory, Cotter Road, Weston Australian Capital Territory 2611, Australia, 6Department of Physics, Texas Tech University, Lubbock, TX 79409, USA, 7US Naval Observatory, P.O. Box 1149, Flagstaff, AZ 86002, USA, 8Max-Planck-Institute für Astronomy, Königstuhl 17, D-69117, Heidelberg, Germany, 9Department of Physics, University of Ljubljana, Jadronska 19, 1000, Ljubljana, Slovenia, 10Department of Astronomy and Astrophysics, Center, 11The Enrico Fermi Institute, University of Chicago, Chicago, IL, 60637, USA The halo of the Milky Way provides unique elemental abundance and kinematic information on the first objects to form in the Universe, which can be used to tightly constrain models of galaxy formation and evolution. Although the halo was once considered a single component, evidence for is dichotomy has slowly emerged in recent years from inspection of small samples of halo objects. Here we show that the halo is indeed clearly divisible into two broadly overlapping structural components -- an inner and an outer halo – that exhibit different spatial density profiles, stellar orbits and stellar metallicities (abundances of elements heavier than helium). -
Near-Field Cosmology with Extremely Metal-Poor Stars
AA53CH16-Frebel ARI 29 July 2015 12:54 Near-Field Cosmology with Extremely Metal-Poor Stars Anna Frebel1 and John E. Norris2 1Department of Physics and Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139; email: [email protected] 2Research School of Astronomy & Astrophysics, The Australian National University, Mount Stromlo Observatory, Weston, Australian Capital Territory 2611, Australia; email: [email protected] Annu. Rev. Astron. Astrophys. 2015. 53:631–88 Keywords The Annual Review of Astronomy and Astrophysics is stellar abundances, stellar evolution, stellar populations, Population II, online at astro.annualreviews.org Galactic halo, metal-poor stars, carbon-enhanced metal-poor stars, dwarf This article’s doi: galaxies, Population III, first stars, galaxy formation, early Universe, 10.1146/annurev-astro-082214-122423 cosmology Copyright c 2015 by Annual Reviews. All rights reserved Abstract The oldest, most metal-poor stars in the Galactic halo and satellite dwarf galaxies present an opportunity to explore the chemical and physical condi- tions of the earliest star-forming environments in the Universe. We review Access provided by California Institute of Technology on 01/11/17. For personal use only. the fields of stellar archaeology and dwarf galaxy archaeology by examin- Annu. Rev. Astron. Astrophys. 2015.53:631-688. Downloaded from www.annualreviews.org ing the chemical abundance measurements of various elements in extremely metal-poor stars. Focus on the carbon-rich and carbon-normal halo star populations illustrates how these provide insight into the Population III star progenitors responsible for the first metal enrichment events. We extend the discussion to near-field cosmology, which is concerned with the forma- tion of the first stars and galaxies, and how metal-poor stars can be used to constrain these processes. -
A Complete Spectroscopic Survey of the Milky Way Satellite Segue 1: the Darkest Galaxy
Haverford College Haverford Scholarship Faculty Publications Astronomy 2011 A Complete Spectroscopic Survey of the Milky Way Satellite Segue 1: The Darkest Galaxy Joshua D. Simon Marla Geha Quinn E. Minor Beth Willman Haverford College Follow this and additional works at: https://scholarship.haverford.edu/astronomy_facpubs Repository Citation A Complete Spectroscopic Survey of the Milky Way satellite Segue 1: Dark matter content, stellar membership and binary properties from a Bayesian analysis - Martinez, Gregory D. et al. Astrophys.J. 738 (2011) 55 arXiv:1008.4585 [astro-ph.GA] This Journal Article is brought to you for free and open access by the Astronomy at Haverford Scholarship. It has been accepted for inclusion in Faculty Publications by an authorized administrator of Haverford Scholarship. For more information, please contact [email protected]. The Astrophysical Journal, 733:46 (20pp), 2011 May 20 doi:10.1088/0004-637X/733/1/46 C 2011. The American Astronomical Society. All rights reserved. Printed in the U.S.A. A COMPLETE SPECTROSCOPIC SURVEY OF THE MILKY WAY SATELLITE SEGUE 1: THE DARKEST GALAXY∗ Joshua D. Simon1, Marla Geha2, Quinn E. Minor3, Gregory D. Martinez3, Evan N. Kirby4,8, James S. Bullock3, Manoj Kaplinghat3, Louis E. Strigari5,8, Beth Willman6, Philip I. Choi7, Erik J. Tollerud3, and Joe Wolf3 1 Observatories of the Carnegie Institution of Washington, 813 Santa Barbara Street, Pasadena, CA 91101, USA; [email protected] 2 Astronomy Department, Yale University, New Haven, CT 06520, USA; [email protected] -
Is There Tension Between Observed Small Scale Structure and Cold Dark Matter?
Is there tension between observed small scale structure and cold dark matter? Louis Strigari Stanford University Cosmic Frontier 2013 March 8, 2013 Predictions of the standard Cold Dark Matter model 26 3 1 1. Density profiles rise towards the centersσannv 3of 10galaxies− cm s− (1) h i' ⇥ ⇢ Universal for all halo masses ⇢(r)= s (2) (r/r )(1 + r/r )2 Navarro-Frenk-White (NFW) model s s 2. Abundance of ‘sub-structure’ (sub-halos) in galaxies Sub-halos comprise few percent of total halo mass Most of mass contained in highest- mass sub-halos Subhalo Mass Function Mass[Solar mass] 1 Problems with the standard Cold Dark Matter model 1. Density of dark matter halos: Faint, dark matter-dominated galaxies appear less dense that predicted in simulations General arguments: Kleyna et al. MNRAS 2003, 2004;Goerdt et al. APJ2006; de Blok et al. AJ 2008 Dwarf spheroidals: Gilmore et al. APJ 2007; Walker & Penarrubia et al. APJ 2011; Angello & Evans APJ 2012 2. ‘Missing satellites problem’: Simulations have more dark matter subhalos than there are observed dwarf satellite galaxies Earilest papers: Kauffmann et al. 1993; Klypin et al. 1999; Moore et al. 1999 Solutions to the issues in Cold Dark Matter 1. The theory is wrong i) Not enough physics in theory/simulations (Talks yesterday by M. Boylan-Kolchin, M. Kuhlen) [Wadepuhl & Springel MNRAS 2011; Parry et al. MRNAS 2011; Pontzen & Governato MRNAS 2012; Brooks et al. ApJ 2012] ii) Cosmology/dark matter is wrong (Talk yesterday by A. Peter) 2. The data is wrong i) Kinematics of dwarf spheroidals (dSphs) are more difficult than assumed ii) Counting satellites a) Many more faint satellites around the Milky Way b) Milky Way is an oddball [Liu et al. -
Dwarf Galaxies 1 Planck “Merger Tree” Hierarchical Structure Formation
04.04.2019 Grebel: Dwarf Galaxies 1 Planck “Merger Tree” Hierarchical Structure Formation q Larger structures form q through successive Illustris q mergers of smaller simulation q structures. q If baryons are Time q involved: Observable q signatures of past merger q events may be retained. ➙ Dwarf galaxies as building blocks of massive galaxies. Potentially traceable; esp. in galactic halos. Fundamental scenario: q Surviving dwarfs: Fossils of galaxy formation q and evolution. Large structures form through numerous mergers of smaller ones. 04.04.2019 Grebel: Dwarf Galaxies 2 Satellite Disruption and Accretion Satellite disruption: q may lead to tidal q stripping (up to 90% q of the satellite’s original q stellar mass may be lost, q but remnant may survive), or q to complete disruption and q ultimately satellite accretion. Harding q More massive satellites experience Stellar tidal streams r r q higher dynamical friction dV M ρ V from different dwarf ∝ − r 3 galaxy accretion q and sink more rapidly. dt V events lead to ➙ Due to the mass-metallicity relation, expect a highly sub- q more metal-rich stars to end up at smaller radii. structured halo. 04.04.2019 € Grebel: Dwarf Galaxies Johnston 3 De Lucia & Helmi 2008; Cooper et al. 2010 accreted stars (ex situ) in-situ stars Stellar Halo Origins q Stellar halos composed in part of q accreted stars and in part of stars q formed in situ. Rodriguez- q Halos grow from “from inside out”. Gomez et al. 2016 q Wide variety of satellite accretion histories from smooth growth to discrete events. -
Astro2020 Science White Paper the Multidimensional Milky Way
Astro2020 Science White Paper The Multidimensional Milky Way Thematic Areas: Planetary Systems Star and Planet Formation Formation and Evolution of Compact Objects 3Cosmology and Fundamental Physics 3Stars and Stellar Evolution 3Resolved Stellar Populations and their Environments 3Galaxy Evolution Multi-Messenger Astronomy and Astrophysics Principal Author: Name: Robyn Sanderson Institution: University of Pennsylvania / Flatiron Institute Email: [email protected] Co-authors (affiliations after text): Jeffrey L. Carlin1, Emily C. Cunningham2, Nicolas Garavito-Camargo3, Puragra Guhathakurta2, Kathryn V. Johnston4,5, Chervin F. P. Laporte6, Ting S. Li7,8, S. Tony Sohn9 Endorsers (affiliations after text): From the WFIRST Astrometry Working Group: Jay Anderson9, Andrea Bellini9, David P. Bennett10, Stefano Casertano9, S. Michael Fall9, Mattia Libralato9, Sangeeta Malhotra10, Leonidas A. Moustakas11, Jason Rhodes11 Other Endorsers: Lee Armus12, Yumi Choi13,14, Andres del Pino9, Elena D’Onghia15, Mark Fardal9, Karoline M. Gilbert9, Carl J. Grillmair12, Nitya Kallivayalil16, Evan N. Kirby17, Jing Li18, Jennifer L. Marshall19, Adrian M. Price-Whelan20, Elena Sacchi9, David N. Spergel5,20, Monica Valluri21, Roeland P. van der Marel9 Abstract: Studying our Galaxy, the Milky Way (MW), gives us a close-up view of the inter- play between cosmology, dark matter, and galaxy formation. In the next decade our under- standing of the MW’s dynamics, stellar populations, and structure will undergo a revolution thanks to planned and proposed astrometric, spectroscopic and photometric surveys, build- ing on recent advances by the Gaia astrometric survey. Together, these new efforts will mea- sure three-dimensional positions and velocities and numerous chemical abundances for stars arXiv:1903.07641v1 [astro-ph.GA] 18 Mar 2019 to the MW’s edge and well into the Local Group, leading to a complete multidimensional view of our Galaxy. -
Arxiv:2104.09523V2 [Astro-Ph.GA] 20 Jul 2021
Accepted in The Astrophysical Journal Preprint typeset using LATEX style emulateapj v. 01/23/15 EVIDENCE OF A DWARF GALAXY STREAM POPULATING THE INNER MILKY WAY HALO Khyati Malhan1, Zhen Yuan2, Rodrigo A. Ibata2, Anke Arentsen2, Michele Bellazzini3, Nicolas F. Martin2,4 Accepted in The Astrophysical Journal ABSTRACT Stellar streams produced from dwarf galaxies provide direct evidence of the hierarchical formation of the Milky Way. Here, we present the first comprehensive study of the \LMS-1" stellar stream, that we detect by searching for wide streams in the Gaia EDR3 dataset using the STREAMFINDER algorithm. This stream was recently discovered by Yuan et al. (2020). We detect LMS-1 as a 60◦ long stream to the north of the Galactic bulge, at a distance of ∼ 20 kpc from the Sun, together with additional components that suggest that the overall stream is completely wrapped around the inner Galaxy. Using spectroscopic measurements from LAMOST, SDSS and APOGEE, we infer that the stream is very metal poor (h[Fe=H]i = −2:1) with a significant metallicity dispersion (σ[Fe=H] = 0:4), −1 and it possesses a large radial velocity dispersion (σv = 20 ± 4 km s ). These estimates together imply that LMS-1 is a dwarf galaxy stream. The orbit of LMS-1 is close to polar, with an inclination of 75◦ to the Galactic plane. Both the orbit and metallicity of LMS-1 are remarkably similar to the globular clusters NGC 5053, NGC 5024 and the stellar stream \Indus". These findings make LMS-1 an important contributor to the stellar population of the inner Milky Way halo. -
A Kinematically Selected, Metal-Poor Spheroid in the Outskirts of M31 S
Submitted to ApJ: A Preprint typeset using LTEX style emulateapj v. 11/26/04 A KINEMATICALLY SELECTED, METAL-POOR SPHEROID IN THE OUTSKIRTS OF M31 S. C. Chapman1, R. Ibata2, G. F. Lewis3, A. M. N. Ferguson4, M. Irwin5, A. McConnachie6, N. Tanvir7 Submitted to ApJ: ABSTRACT We present evidence for a metal-poor, [Fe/H]∼ −1.4 ± 0.2 dex, stellar component detectable at radii from 10kpc to 70kpc, in our nearest giant spiral neighbor, the Andromeda galaxy. This metal- poor sample underlies the recently-discovered extended rotating component, and has no detected metallicity gradient. This discovery uses a large sample of 9776 radial velocities of Red Giant Branch (RGB) stars obtained with the Keck-II telescope and DEIMOS spectrograph, with 827 stars isolated kinematically to lie in the spheroid component by windowing out the extended rotating component which dominates the photometric profile of Andromeda out to >50 kpc (de-projected). The stars lie in 54 spectroscopic fields spread over an 8 square degree region, and are expected to fairly sample the stellar halo region to a radius of >70 kpc. The spheroid sample shows no significant evidence for rotation. Fitting a simple model in which the velocity dispersion of the component decreases with radius, we find a central velocity dispersion of 152kms−1 decreasing by −0.90kms−1/ kpc. By fitting a cosmologically-motivated NFW halo model to the spheroid stars we constrain the virial mass of M31 11 to be greater than 9.0 × 10 M with 99% confidence. The properties of this halo component are very similar to that found in our Milky Way, revealing that these roughly equal mass galaxies may have led similar accretion and evolutionary paths in the early Universe. -
The Correlation Between Galaxy Growth and Dark Matter Halo Assembly from Z = 0 − 10
MNRAS 000, 000–000 (2019) Preprint 30 July 2019 Compiled using MNRAS LATEX style file v3.0 UNIVERSEMACHINE: The Correlation between Galaxy Growth and Dark Matter Halo Assembly from z = 0 − 10 Peter Behroozi1,? Risa H. Wechsler2;3, Andrew P. Hearin4, Charlie Conroy5 1 Department of Astronomy and Steward Observatory, University of Arizona, Tucson, AZ 85721, USA 2 Kavli Institute for Particle Astrophysics and Cosmology and Department of Physics, Stanford University, Stanford, CA 94305, USA 3 Department of Particle Physics and Astrophysics, SLAC National Accelerator Laboratory, Stanford, CA 94305, USA 4 High-Energy Physics Division, Argonne National Laboratory, Argonne, IL 60439, USA 5 Department of Astronomy, Harvard University, Cambridge, MA 02138, USA Released 30 July 2019 ABSTRACT We present a method to flexibly and self-consistently determine individual galaxies’ star for- mation rates (SFRs) from their host haloes’ potential well depths, assembly histories, and red- shifts. The method is constrained by galaxies’ observed stellar mass functions, SFRs (specific and cosmic), quenched fractions, UV luminosity functions, UV–stellar mass relations, IRX– UV relations, auto- and cross-correlation functions (including quenched and star-forming sub- samples), and quenching dependence on environment; each observable is reproduced over the full redshift range available, up to 0 < z < 10. Key findings include: galaxy assembly corre- lates strongly with halo assembly; quenching correlates strongly with halo mass; quenched fractions at fixed halo mass decrease with increasing redshift; massive quenched galaxies re- side in higher-mass haloes than star-forming galaxies at fixed galaxy mass; star-forming and quenched galaxies’ star formation histories at fixed mass differ most at z < 0:5; satellites have large scatter in quenching timescales after infall, and have modestly higher quenched frac- tions than central galaxies; Planck cosmologies result in up to 0:3 dex lower stellar—halo mass ratios at early times; and, nonetheless, stellar mass–halo mass ratios rise at z > 5. -
Star Clusters E NCYCLOPEDIA of a STRONOMY and a STROPHYSICS
Star Clusters E NCYCLOPEDIA OF A STRONOMY AND A STROPHYSICS Star Clusters the Galaxy can be used to derive the cluster distance, independently of parallax measurements. Even a small telescope shows obvious local concentrations Afinal category of clusters has recently been identified of stars scattered around the sky. These star clusters are based on observations with infrared detectors. These are not chance juxtapositions of unrelated stars. They are, the embedded clusters—star clusters still in the process of instead, physically associated groups of stars, moving formation, and still embedded in the clouds out of which together through the Galaxy. The stars in a cluster are they formed. Because it is possible to see through the dust held together either permanently or temporarily by their much better at infrared wavelengths than in the optical, mutual gravitational attraction. these clusters have suddenly become observable. The classic, and best known, example of a star cluster Star clusters are of considerable astrophysical impor- is the Pleiades, visible in the evening sky in early winter tance to probe models of stellar evolution and dynamics, (from the northern hemisphere) as a group of 7–10 stars explore the star formation process, calibrate the extragalac- (depending on one’s eyesight). More than 600 Pleiades tic distance scale and most importantly to measure the age members have been identified telescopically. and evolution of the Galaxy. Clusters are generally distinguished as being either Definition of a star cluster—cluster catalogs GALACTIC OPEN CLUSTERS or GLOBULAR CLUSTERS, corresponding Just what is a cluster? How many stars does it take to to their appearance as seen through a moderate-aperture make a cluster? Trumpler in 1930 defined open clusters telescope. -
Galactic Archaeology with the Oldest Stars in the Milky Way
Galactic Archaeology with the oldest stars in the Milky Way Anke Arentsen Leibniz-Institut für Astrophysik Potsdam (AIP) Kumulative dissertation zur Erlangung des akademischen Grades doctor rerum naturalium (Dr. rer. nat.) in der Wissenschaftsdisziplin Astrophysik Eingereicht an der Mathematisch-Naturwissenschaftlichen Fakultät Institut für Physik und Astronomie der Universität Potsdam und das Leibniz-Institut für Astrophysik Potsdam (AIP) Potsdam, 16.09.2020 Betreuer: Dr. Else Starkenburg/Prof. Dr. Matthias Steinmetz 1. Gutachter: Dr. Else Starkenburg Leibniz-Institut für Astrophysik Potsdam 2. Gutachter: Prof. Dr. Matthias Steinmetz Leibniz-Institut für Astrophysik Potsdam/Universität Potsdam 3. Gutachter: Prof. Dr. Norbert Christlieb Zentrum für Astronomie der Universität Heidelberg/Landessternwarte Published online on the Publication Server of the University of Potsdam: https://doi.org/10.25932/publishup-47602 https://nbn-resolving.org/urn:nbn:de:kobv:517-opus4-476022 “... it is difficult to resist the impression that the evolution of „ the stellar universe proceeds at a slow majestic pace ...” — Sir A. S. Eddington (The internal constitution of the stars, 1920) Contents Summary/Zusammenfassung i 1 Introduction 1 1.1 What can we learn from metal-poor stars about the First Stars? . .4 1.1.1 Using observations to set constraints on the First Stars . .5 1.1.2 Models of CEMP star origins . .6 1.1.3 3D/NLTE effects on the carbon abundance . .7 1.1.4 Contribution of this thesis to the field . .9 1.2 Galactic archaeology with pristine stars . .9 1.2.1 How to find metal-poor stars . 10 1.2.2 Photometric surveys . 10 1.2.3 Recent metal-poor Milky Way results .